JPH08203652A - High temperature superconducting junction manufacturing method - Google Patents
High temperature superconducting junction manufacturing methodInfo
- Publication number
- JPH08203652A JPH08203652A JP6324858A JP32485894A JPH08203652A JP H08203652 A JPH08203652 A JP H08203652A JP 6324858 A JP6324858 A JP 6324858A JP 32485894 A JP32485894 A JP 32485894A JP H08203652 A JPH08203652 A JP H08203652A
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- temperature superconductor
- high temperature
- precursor
- superconducting
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment
Landscapes
- Manufacturing Of Electrical Connectors (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Abstract
(57)【要約】
【目的】 接合する高温超電導体の超電導特性を低下さ
せることなく、また接合部分の超電導体結晶も高く配向
させて、良好な超電導接合を得る高温超電導接合体の製
造法を提供する。
【構成】 基材(銀板)1上に形成された高温超電導体
2、2′同士を接合する方法において、接合する高温超
電導体2、2′間に高温超電導体前駆体3を介在させ、
基材1上に形成された高温超電導体結晶が分解及び/又
は溶融せず、かつ高温超電導体前駆体3の一部が溶融
し、その後高温超電導体前駆体3全体が結晶化する温度
で加熱して高温超電導体2、2′同士を接合する高温超
電導接合体の製造法。
(57) [Abstract] [Purpose] A method for producing a high-temperature superconducting junction, which does not deteriorate the superconducting properties of the high-temperature superconductor to be joined and also orients the superconducting crystal in the joining portion to a high orientation, to obtain a good superconducting junction provide. In a method of joining high temperature superconductors 2 and 2'formed on a base material (silver plate) 1, a high temperature superconductor precursor 3 is interposed between the high temperature superconductors 2 and 2'to be joined,
Heating at a temperature at which the high-temperature superconductor crystal formed on the base material 1 does not decompose and / or melt, and a part of the high-temperature superconductor precursor 3 melts, and then the entire high-temperature superconductor precursor 3 crystallizes Then, a method of manufacturing a high temperature superconducting joined body for joining the high temperature superconductors 2, 2'to each other.
Description
【0001】[0001]
【産業上の利用分野】本発明は、製造が比較的容易な小
型の高温超電導体から大型の高温超電導体を製造するの
に有効な高温超電導接合体の製造法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for producing a high temperature superconducting assembly which is effective for producing a large high temperature superconductor from a small high temperature superconductor which is relatively easy to produce.
【0002】[0002]
【従来の技術】高温超電導体は、焼成が可能な温度幅が
狭く、また機械的強度が低いため機械加工が困難である
などの理由で大型又は複雑な形状のものを一体で製造で
きないという問題点がある。この問題点に対して、あら
かじめ適当な大きさ又は形状の金属、セラミックス等の
基材を作製し、この基材の表面に高温超電導体を焼き付
け、基材及び高温超電導体同士を接合して一体化する方
法が考えられている。基材及び高温超電導体同士を接合
する方法としては、例えば特開平5−145267号公
報に示されるように、基材上に形成した高温超電導体同
士を接触させてその接合部分を局所的に加熱して接合し
たり、基材と高温超電導体との複合基材の各層それぞれ
を接合する方法が提案されている。2. Description of the Related Art A high temperature superconductor has a problem that it cannot be integrally manufactured in a large size or in a complicated shape because it is difficult to machine because it has a narrow temperature range in which it can be fired and has low mechanical strength. There is a point. In order to solve this problem, a base material such as metal or ceramics having an appropriate size or shape is prepared in advance, a high-temperature superconductor is baked on the surface of this base material, and the base material and the high-temperature superconductor are joined together to form an integrated body. The method to make it is considered. As a method of joining the base material and the high-temperature superconductor to each other, for example, as shown in JP-A-5-145267, the high-temperature superconductors formed on the base material are brought into contact with each other to locally heat the joined portion. Then, a method of joining each layer of the composite base material of the base material and the high temperature superconductor has been proposed.
【0003】[0003]
【発明が解決しようとする課題】しかしながら、高温超
電導体結晶は緻密に焼結しにくい性質のため、高温超電
導体を単に加熱焼成する方法では多孔質のままになり、
高温超電導体結晶間に残存する隙間によって良好な超電
導接合(超電導特性が途中で遮断されずに接続されるよ
うにした接合)が困難であり、良好な超電導接合を得よ
うとして加熱温度を上昇させると高温超電導体結晶が分
解又は溶融したり、基材と反応するなどの問題点が生じ
る。However, since the high-temperature superconductor crystal is difficult to be densely sintered, the high-temperature superconductor is simply porous by heating and remains porous.
Good superconducting joining (joining in which the superconducting characteristics are connected without being interrupted in the middle) is difficult due to the gaps remaining between the high-temperature superconducting crystals, and the heating temperature is raised in order to obtain good superconducting joining. Therefore, problems such as decomposition or melting of the high-temperature superconductor crystal and reaction with the base material occur.
【0004】即ち高温超電導体は、焼結しにくく、また
極めて狭い温度条件で結晶生成及び成長するものであ
り、接合部分に超電導体結晶粉を塗布し、これを加熱し
て接合部分を緻密化させて超電導接合をしようとする
と、高温の処理温度が必要になるため、周囲の高温超電
導体がその温度により相変化して超電導体でなくなった
り、高温超電導体以外の結晶が生成するなどにより特性
を低下させてしまうという問題点が生じる。That is, a high-temperature superconductor is hard to sinter, and crystals are formed and grow under extremely narrow temperature conditions. Superconductor crystal powder is applied to the joint portion and heated to densify the joint portion. If you try to make superconducting joints by doing so, a high processing temperature is required, so the surrounding high-temperature superconductor changes its phase and disappears as a superconductor, or crystals other than high-temperature superconductor are generated. However, there is a problem in that
【0005】例えば、良好な超電導特性が得られる方法
として知られている部分溶融法は、高温超電導体結晶が
ある結晶と融液とに分解して緻密化し、次に冷却して再
度高温超電導体結晶に結晶化させる方法であるが、これ
を加熱接合の条件に適用しようとすると、その部分溶融
で生じた融液で周囲の高温超電導体も分解してしまう。
従って部分的な加熱焼成で接合部分だけは超電導体化し
て良好な接合が得られても、周囲の高温超電導体は特性
の低下又は非超電導化するため結局良好な超電導接合と
はならない。特性の低下を避けるには、全体を焼成する
のと同じような精密な焼成技術が必要であるが、全体を
焼成するのでは接合する意義が無くなる。For example, the partial melting method, which is known as a method for obtaining good superconducting characteristics, is decomposed into a crystal having a high-temperature superconductor crystal and a melt to densify it, and then cooled to re-produce the high-temperature superconductor. This is a method of crystallizing into crystals, but if this is applied to the conditions of heat bonding, the surrounding high temperature superconductor will also be decomposed by the melt generated by the partial melting.
Therefore, even if only the joint portion is made into a superconductor by a partial heating and firing and a good joint is obtained, the surrounding high temperature superconductor is deteriorated in characteristics or becomes non-superconducting, so that a good superconducting joint is not eventually obtained. In order to avoid the deterioration of the characteristics, it is necessary to use a precise firing technique similar to that for firing the whole, but if the whole is fired, the meaning of joining is lost.
【0006】本発明は、上記のような問題点が生じない
よう、接合する高温超電導体を分解及び/又は溶融する
温度に加熱しないで、しかも望ましい板状の高温超電導
体結晶が基材表面に並行に配向した状態になる良好な超
電導体接合が得られる高温超電導接合体の製造法を提供
するものである。In order to avoid the above problems, the present invention does not heat the high temperature superconductor to be joined to a temperature at which it decomposes and / or melts, and a desirable plate-shaped high temperature superconductor crystal is formed on the substrate surface. It is intended to provide a method for producing a high-temperature superconducting joint, which can obtain a good superconducting joint that is oriented in parallel.
【0007】[0007]
【課題を解決するための手段】本発明者らは、基材上に
形成された高温超電導体同士を接合するため、高温超電
導体結晶が分解する温度より低い温度で、各種の高温超
電導体前駆体が示す挙動を詳細に調査した結果、高温超
電導体前駆体は加熱すると高温超電導体結晶を析出する
が、その作製法によっては結晶化する前に溶融して緻密
な組織が得られることを見出した。溶融する例をさらに
検討した結果、溶融するのは高温超電導体の組成からは
ずれた組成物であり、溶融しながら近傍の組織を徐々に
溶かし込むことで高温超電導体の組成になり、高温超電
導体結晶を析出する。即ち溶融などの方法で粉体の粒子
単位で均一な組成にすると加熱工程で溶融しにくくな
り、高温超電導体の組成になり、高温超電導体結晶が析
出することを見出し本発明を完成するに至った。Means for Solving the Problems In order to bond the high temperature superconductors formed on the substrate, the present inventors have made various high temperature superconductor precursors at a temperature lower than the temperature at which the high temperature superconductor crystals decompose. As a result of detailed investigation of the behavior of the body, it was found that the high-temperature superconductor precursor precipitates high-temperature superconductor crystals when heated, but depending on the method of preparation, it melts before crystallization to obtain a dense structure. It was As a result of further studying the example of melting, it is the composition that deviates from the composition of the high-temperature superconductor.By gradually melting the nearby structure while melting, it becomes the composition of the high-temperature superconductor. Precipitate crystals. That is, when a uniform composition is obtained for each particle of the powder by a method such as melting, it becomes difficult to melt in the heating step, the composition becomes a high-temperature superconductor, and high-temperature superconductor crystals are found to be deposited, and the present invention is completed. It was
【0008】本発明は基材上に形成された高温超電導体
同士を接合する方法において、接合する高温超電導体間
に高温超電導体前駆体を介在させ、基材上に形成された
高温超電導体結晶が分解及び/又は溶融せず、かつ高温
超電導体前駆体の一部が溶融し、その後高温超電導体前
駆体全体が結晶化する温度で加熱して高温超電導体同士
を接合する高温超電導接合体の製造法並びに貴金属板上
に高温超電導体前駆体の膜を形成して複合材料を得、次
いで該複合材料の高温超電導体前駆体の膜の部分を下側
にして接合する高温超電導体間の上部に載置した後、基
材上に形成された高温超電導体結晶が分解及び/又は溶
融せず、かつ載置した高温超電導体前駆体の一部が溶融
し、その後高温超電導体前駆体全体が結晶化する温度で
加熱して高温超電導体同士を接合する高温超電導接合体
の製造法に関する。The present invention relates to a method for joining high-temperature superconductors formed on a base material, wherein a high-temperature superconductor precursor is interposed between the high-temperature superconductors to be joined, and a high-temperature superconductor crystal formed on the base material. Of a high-temperature superconducting joint in which the high-temperature superconductor precursor is not melted and / or melted, and a part of the high-temperature superconductor precursor is melted Manufacturing method and high temperature superconductor precursor film is formed on a noble metal plate to obtain a composite material, and then the upper part between the high temperature superconductors to be joined with the high temperature superconductor precursor film part of the composite material facing downward The high temperature superconductor crystal formed on the base material does not decompose and / or melt after being placed on the substrate, and a part of the placed high temperature superconductor precursor is melted, and then the whole high temperature superconductor precursor is High temperature superheated by heating at the crystallization temperature HTS assembly for joining the body to each other about the preparation of.
【0009】本発明において、基材の種類、組成につい
ては特に制限はないが、高温超電導体の加熱温度に耐え
られ、かつ機械的強度を有する材料、例えばインコネ
ル、ステンレス、ハステロイ等の金属基材、セラミック
スなどを用いることが好ましく、このうち加工の容易
さ、熱膨張率等の点からインコネルを用いることが好ま
しい。なお加熱工程で高温超電導体が基材と望ましくな
い反応を起こすおそれがある場合は、基材の表面に銀、
金等の貴金属の膜や酸化マグネシウムの膜を形成して用
いられる。貴金属の膜を形成する場合、下地金属として
銅又は銅合金の膜を形成しておけば、貴金属の膜が剥離
するのを防止できるので好ましい。In the present invention, the kind and composition of the base material is not particularly limited, but a material that can withstand the heating temperature of the high temperature superconductor and has mechanical strength, for example, a metal base material such as Inconel, stainless steel or Hastelloy. , Ceramics and the like are preferably used, and of these, Inconel is preferably used in terms of easiness of processing, thermal expansion coefficient and the like. If the high-temperature superconductor may cause an undesirable reaction with the base material in the heating step, silver on the surface of the base material,
It is used by forming a film of noble metal such as gold or a film of magnesium oxide. When forming a film of a noble metal, it is preferable to form a film of copper or a copper alloy as a base metal because the film of the noble metal can be prevented from peeling off.
【0010】高温超電導体前駆体は、高温超電導体の組
成になるように酸化物又は炭酸塩などの原料を秤量、混
合、仮焼したもの若しくは前記原料を秤量、混合、仮焼
及び/又は溶融後粉砕した2種類以上の粉体をさらに混
合したものを用いることが好ましい。該高温超電導体前
駆体は、高温超電導体の分解温度以下で溶融し、次いで
高温超電導体結晶を生成させるために、各組成からなる
粒子が均一に分散された微粉を用いることが好ましく、
その平均粒径は溶融し易く、取り扱いの容易さから1〜
15μmであることが好ましく、3〜10μmであれば
さらに好ましい。The high temperature superconductor precursor is a material obtained by weighing, mixing, and calcining raw materials such as oxides and carbonates so as to have the composition of the high temperature superconductor, or weighing, mixing, calcining and / or melting the raw materials. It is preferable to use a mixture of two or more kinds of powders that have been post-pulverized. The high-temperature superconductor precursor is preferably melted at a temperature below the decomposition temperature of the high-temperature superconductor, and in order to generate high-temperature superconductor crystals, it is preferable to use fine powder in which particles of each composition are uniformly dispersed,
Its average particle size is easy to melt, and it is easy to handle.
It is preferably 15 μm, and more preferably 3 to 10 μm.
【0011】接合する高温超電導体は介在させる高温超
電導体前駆体とは異なり、各原料を混合した後、溶融な
どの方法で粉体の粒子単位まで均一な組成にすれば、高
温超電導体の結晶含有率が高く、加熱工程で異相の生成
等の異常な挙動が低減できるため好ましい。また銀を添
加すれば結晶の生成を促進するなどの効果があり好まし
い。The high-temperature superconductor to be joined is different from the high-temperature superconductor precursor to be interposed, and when the raw materials are mixed and then made into a uniform composition up to the particle unit of the powder by a method such as melting, the crystal of the high-temperature superconductor is formed. It is preferable because the content is high and abnormal behavior such as generation of a different phase can be reduced in the heating step. Further, addition of silver is preferable because it has an effect of promoting the generation of crystals.
【0012】高温超電導体前駆体に、接合する高温超電
導体と同じ結晶構造を有する高温超電導体結晶粉を50
重量%含有させれば、結晶が成長し易く、成長の方向も
制御でき、また安価に製造できるので好ましい。To the high temperature superconductor precursor, 50 high temperature superconductor crystal powder having the same crystal structure as the high temperature superconductor to be joined is added.
If the content is wt%, the crystal is easy to grow, the growth direction can be controlled, and the production can be performed at low cost, which is preferable.
【0013】高温超電導体前駆体を高温超電導体間に介
在させる方法については特に制限はなく、例えば高温超
電導体前駆体の粉末をスプレーで吹き付けたり、スラリ
ー状又はペースト化した液状の高温超電導体前駆体を塗
布したり、シート状に成形した高温超電導体前駆体を張
り合わせたりする等の方法で介在させることができる。
高温超電導体同士は重ねてもよく、また横に並べて高温
超電導体前駆体を高温超電導体間に介在させてもよい。There is no particular limitation on the method for interposing the high temperature superconductor precursor between the high temperature superconductors. For example, powder of the high temperature superconductor precursor is sprayed, or a liquid high temperature superconductor precursor in the form of a slurry or a paste. It can be intervened by a method of applying a body or laminating a sheet-shaped high temperature superconductor precursor.
The high temperature superconductors may be overlapped with each other, or the high temperature superconductor precursors may be arranged side by side and interposed between the high temperature superconductors.
【0014】高温超電導体前駆体の膜を形成する貴金属
板としては、銀または銀を主成分とする合金板を用いる
ことが好ましい。高温超電導体前駆体の膜の形成方法に
ついても特に制限はないが、シート状に成形した高温超
電導体前駆体を貴金属板上に加圧して成形したものを接
合部に張り合わせれば高温超電導体結晶が配向し、かつ
高温超電導体結晶の成長方向が制御できるので好まし
い。As the noble metal plate forming the film of the high temperature superconductor precursor, silver or an alloy plate containing silver as a main component is preferably used. There is no particular limitation on the method of forming the film of the high temperature superconductor precursor, but if the high temperature superconductor precursor formed into a sheet is pressed onto a noble metal plate and the formed product is bonded to the joint, the high temperature superconductor crystal is formed. Are preferred, and the growth direction of the high-temperature superconductor crystal can be controlled, which is preferable.
【0015】高温超電導体前駆体及び接合する高温超電
導体に用いられる超電導体の種類については特に制限は
なく、例えばBi系高温超電導体、Y系高温超電導体、
Tl系高温超電導体等が適用できるが本発明においては
Bi系高温超電導体を用いれば良好な超電導接合が得ら
れ易いので好ましい。なおBi系高温超電導体には22
12相、2223相等があるが、このうちBi系221
2相が操作し易いうえ、結晶成長速度が比較的大きいの
で好ましい。There is no particular limitation on the kind of the superconductor used for the high temperature superconductor precursor and the high temperature superconductor to be joined. For example, a Bi type high temperature superconductor, a Y type high temperature superconductor,
Although a Tl-based high temperature superconductor or the like can be applied, it is preferable to use a Bi-based high temperature superconductor in the present invention because a good superconducting junction can be easily obtained. 22 for Bi-based high-temperature superconductors
There are 12 phases, 2223 phases, etc. Of these, Bi system 221
The two phases are preferable because they are easy to operate and the crystal growth rate is relatively high.
【0016】高温超電導体同士を接合するための加熱条
件は、基材上に形成された超電導体結晶が分解及び/又
は溶融せず、かつ介在する高温超電導体前駆体の一部が
溶融し、その後高温超電導体前駆体全体が結晶化する温
度で加熱することが必要とされ、これ以外の条件では超
電導接合が困難であったり、超電導特性が低下するなど
の問題点が生じる。なお、加熱に最適の温度は、高温超
電導体前駆体の結晶粒径や周囲の酸素分圧、昇温速度等
の焼成条件により変化するため適宜選定する。焼成雰囲
気は大気中、酸素分圧を制御した雰囲気中で行うことが
好ましい。The heating conditions for joining the high-temperature superconductors to each other are that the superconductor crystals formed on the substrate are not decomposed and / or melted, and a part of the interposing high-temperature superconductor precursor is melted, After that, it is necessary to heat at a temperature at which the entire high temperature superconductor precursor is crystallized, and under other conditions, problems such as difficulty in superconducting bonding and deterioration of superconducting properties occur. The optimum temperature for heating varies depending on the firing conditions such as the crystal grain size of the high-temperature superconductor precursor, the oxygen partial pressure of the surroundings, and the heating rate, and is appropriately selected. The firing atmosphere is preferably atmospheric air or an atmosphere in which the oxygen partial pressure is controlled.
【0017】[0017]
【実施例】以下本発明の実施例を説明する。なお本発明
はこれらに制限されない。 実施例1 純度99.9重量%以上の酸化ビスマス(高純度化学研
究所製、3N)466g、炭酸ストロンチウム(高純度
化学研究所製、3N)295.2g、炭酸カルシウム
(高純度化学研究所製、3N)100.1g及び酸化第
二銅(高純度化学研究所製、3N)159.1gを秤量
し、合成樹脂製ボールミルに直径10mmの合成樹脂製ボ
ール2kg及び蒸留水1kgと共に入れ72時間湿式混合し
た。混合液は100℃で24時間乾燥し、乾燥粉を銀製
容器に移し替えて820℃で5時間仮焼した、仮焼後ら
いかい機で平均粒径が7μmに乾式粉砕して高温超電導
体前駆体(A)を得た。この高温超電導体前駆体(A)
は2212相が約6重量%及び少量の同定できない結晶
を含む非晶質体であった。EXAMPLES Examples of the present invention will be described below. The present invention is not limited to these. Example 1 Bismuth oxide having a purity of 99.9% by weight or more (manufactured by Kojundo Chemical Laboratory, 3N) 466 g, strontium carbonate (manufactured by Kojundo Chemical Laboratory, 3N) 295.2 g, calcium carbonate (manufactured by Kojundo Chemical Laboratory) 3N) 100.1 g and cupric oxide (manufactured by Kojundo Chemical Laboratory, 3N) 159.1 g are weighed and put in a synthetic resin ball mill together with 2 kg of synthetic resin balls having a diameter of 10 mm and 1 kg of distilled water for 72 hours. Mixed. The mixed solution was dried at 100 ° C for 24 hours, the dried powder was transferred to a silver container and calcined at 820 ° C for 5 hours. After calcination, a high temperature superconductor precursor was obtained by dry grinding to an average particle size of 7 μm. The body (A) was obtained. This high temperature superconductor precursor (A)
Was an amorphous body with 2212 phase containing about 6% by weight and a small amount of unidentifiable crystals.
【0018】次に、上記で得た高温超電導体前駆体
(A)をジルコニア容器に入れて、1050℃で2時間
加熱後、内容物を銀板上に流し出して急冷し、さらにら
いかい機で平均粒径8μmに乾式粉砕して溶融粉(A)
を得た。Next, the high temperature superconductor precursor (A) obtained above was placed in a zirconia container and heated at 1050 ° C. for 2 hours, and then the contents were poured onto a silver plate and rapidly cooled. Melt powder (A) by dry pulverization to an average particle size of 8 μm
I got
【0019】次いで溶融粉(A)100重量部にポリビ
ニールブチラール樹脂(積水化学製、商品名BL−2)
5重量部、ジブチルフタレート(和光純薬製、試薬一
級)2重量部及びエチルアルコール(和光純薬製、試薬
一級)15重量部を添加して混合した後、真空脱気して
得られたスラリーを厚さが100μmのポリエステル製
フィルム(東レ製)上に供給し、ドクターブレード法で
シート成形して厚さ150μmのグリーンシート(A)
を得た。Next, 100 parts by weight of the molten powder (A) was mixed with polyvinyl butyral resin (manufactured by Sekisui Chemical Co., Ltd., trade name BL-2).
5 parts by weight, 2 parts by weight of dibutyl phthalate (manufactured by Wako Pure Chemical Industries, reagent first grade) and 15 parts by weight of ethyl alcohol (manufactured by Wako Pure Chemical Industries, reagent first class) were added and mixed, and then vacuum degassing was performed to obtain a slurry. Is supplied onto a polyester film (made by Toray) having a thickness of 100 μm, and the green sheet (A) having a thickness of 150 μm is formed by the doctor blade method.
I got
【0020】この後厚さ0.1mmの銀板上に上記で得た
グリーンシート(A)を60℃で10MPaの条件で熱圧
着し、断面流速5cm/分で空気を流しながら焼成し、結
晶が十分に成長して配向し、かつ平滑な表面になる条件
及び高温超電導体結晶が得られる温度条件を調べた。そ
の結果、最高温度は872〜886℃の範囲で、保持時
間は2時間以内、降温速度は850℃以上では5℃/時
間以下が良好であることを確認した。そこで断面流速5
cm/分で空気を流しながら、883℃に加熱し、30分
間保持した後2℃/時間の速度で850℃まで降温し、
以後100℃/時間の速度で室温まで冷却して銀板上に
高温超電導体を形成した超電導複合体を得た。次いで得
られた超電導複合体の超電導体結晶が溶融する温度を調
べるため、超電導複合体を860〜890℃まで1℃ず
つ温度を変えて20分保持した後に炉外に取り出して、
X線回折法で結晶状態を調べた。その結果、873℃を
越えると含まれていたBi系2212相結晶は消失し、
2201結晶が大量に検出されたことから加熱温度の限
界を873℃とした。Thereafter, the green sheet (A) obtained above was thermocompression-bonded on a silver plate having a thickness of 0.1 mm at 60 ° C. under the condition of 10 MPa, and baked at a cross-sectional flow rate of 5 cm / min while flowing air to crystallize. Were sufficiently grown to be oriented and have a smooth surface, and the temperature conditions under which a high-temperature superconductor crystal was obtained were investigated. As a result, it was confirmed that the maximum temperature was in the range of 872 to 886 ° C, the holding time was within 2 hours, and the cooling rate was 5 ° C / hour or less at 850 ° C or higher. Therefore cross-sectional flow velocity 5
While flowing air at cm / min, heat to 883 ° C, hold for 30 minutes, and then cool to 850 ° C at a rate of 2 ° C / hour,
Then, it was cooled to room temperature at a rate of 100 ° C./hour to obtain a superconducting composite in which a high temperature superconductor was formed on a silver plate. Then, in order to investigate the temperature at which the superconductor crystal of the obtained superconducting composite melts, the superconducting composite was taken out of the furnace after changing the temperature by 1 ° C for 1 minute from 860 to 890 ° C for 20 minutes.
The crystal state was examined by the X-ray diffraction method. As a result, when the temperature exceeds 873 ° C., the contained Bi-based 2212 phase crystal disappears,
Since a large amount of 2201 crystals were detected, the heating temperature limit was set to 873 ° C.
【0021】一方高温超電導体前駆体(A)100重量
部にグリーンシート(A)を得る工程と同様の工程を経
て厚さ170μmのグリーンシート(B)(高温超電導
体前駆体(B))を得た。この後、上記と同様に厚さ0.
1mmの銀板上に上記で得た高温超電導体前駆体(B)を
60℃で10MPaの条件で熱圧着し、断面流速5cm/分で
空気を流しながら焼成し、高温超電導体前駆体(B)の
一部が溶融し、かつ高温超電導体結晶が得られる温度条
件を調べた。その結果、最高温度は865〜875℃の
範囲で、保持時間は2時間以内、降温速度は850℃以
上では5℃/時間以下の降温速度が良好であることを確
認した。On the other hand, a green sheet (B) (high temperature superconductor precursor (B)) having a thickness of 170 μm is obtained through the same steps as the step of obtaining the green sheet (A) in 100 parts by weight of the high temperature superconductor precursor (A). Obtained. After this, the thickness of 0.
The high-temperature superconductor precursor (B) obtained above was thermocompression-bonded on a 1 mm silver plate under the conditions of 60 MPa and 10 MPa, and baked at a cross-sectional flow rate of 5 cm / min while flowing air to obtain a high-temperature superconductor precursor (B). ) Was partially melted and the temperature conditions under which a high-temperature superconductor crystal was obtained were investigated. As a result, it was confirmed that the maximum temperature was in the range of 865 to 875 ° C, the holding time was within 2 hours, and the temperature decreasing rate was 5 ° C / hour or less at 850 ° C or higher.
【0022】次に高温超電導体前駆体(B)の超電導体
結晶が溶融する温度を調べるため、銀板上に載置した高
温超電導体前駆体(B)を860〜890℃まで1℃ず
つ温度を変えて20分保持した後に炉外に取り出して、
X線回折法で結晶状態を調べた。その結果、871℃以
上になると含まれていたBi系2212相結晶は消失
し、2201結晶が大量に検出された。なお高温超電導
体前駆体(B)は870温度以下から急冷しても221
2相と共に多量の2201相が検出され、また868℃
以上の温度で再加熱して除冷すると、超電導体ではない
柱状結晶が大量に生成した。Next, in order to investigate the temperature at which the superconductor crystal of the high temperature superconductor precursor (B) melts, the temperature of the high temperature superconductor precursor (B) placed on a silver plate is increased by 1 ° C. from 860 to 890 ° C. Change and hold for 20 minutes, then take it out of the furnace,
The crystal state was examined by the X-ray diffraction method. As a result, at 871 ° C. or higher, the contained Bi-based 2212 phase crystals disappeared and 2201 crystals were detected in large amounts. The high temperature superconductor precursor (B) is 221 even if it is rapidly cooled from a temperature of 870 or lower.
A large amount of 2201 phase was detected together with 2 phases, and 868 ° C.
When reheated at the above temperature and then cooled, a large amount of columnar crystals that were not superconductors were generated.
【0023】上記で得られた超電導複合体を図1の
(a)及び(b)に示すように突き合わせ、かつ突き合
わせた双方の銀板1、1′の先端部を加締めて固定した
後、銀板1、1′の上部に形成した高温超電導体2、
2′間に、上記で得た高温超電導体前駆体(B)3をブ
チルアルコール(和光純薬製、試薬)を塗布して接着
し、大気中で最高温度が868℃で30分間保持(加熱
処理)し、その後850℃まで15時間かけて降温し、
更に20℃まで5時間かけて冷却して高温超電導接合体
を得た。なお冷却工程で680℃からは雰囲気を窒素雰
囲気に変更した。図1の(b)において4は銀板1、
1′の加締め部である。The superconducting composite obtained above is abutted as shown in FIGS. 1 (a) and 1 (b), and the tips of the abutted silver plates 1, 1'are fixed by caulking. High temperature superconductor 2 formed on the silver plates 1, 1 ',
The high-temperature superconductor precursor (B) 3 obtained above was coated with butyl alcohol (a reagent manufactured by Wako Pure Chemical Industries, Ltd.) between the 2'and adhered, and the maximum temperature was kept at 868 ° C for 30 minutes in the atmosphere (heating Treatment) and then lowering the temperature to 850 ° C. over 15 hours,
Furthermore, it cooled to 20 degreeC over 5 hours, and obtained the high temperature superconducting joined body. In the cooling step, the atmosphere was changed to a nitrogen atmosphere from 680 ° C. In FIG. 1B, 4 is a silver plate 1,
It is a crimping portion 1 '.
【0024】上記で得た高温超電導接合体の接合部とそ
の周辺を顕微鏡及びX線回折法で観察すると共に4端子
法で臨界電流密度(以下Jcとする)を測定した。その
結果、高温超電導体の液体窒素温度77.3KでのJc
は、接合前は8600A/mm2及び接合後は7400A/mm2
であり、また接合部分のJcは、接合部分の超電導体膜
厚さで算出した値で6200A/mm2であった。また接合
部の接合状態は、高温超電導体の流動による異常な凹
凸、発泡、異相等がなく、接合面と並行に良く配向され
ており、良好な接合が得られていた。The joint part and its periphery of the high temperature superconducting joint body obtained above were observed by a microscope and an X-ray diffraction method, and the critical current density (hereinafter referred to as Jc) was measured by a four-terminal method. As a result, Jc at a liquid nitrogen temperature of 77.3K of the high temperature superconductor
It is joined before the 8600A / mm 2 and after the bonding 7400A / mm 2
Further, Jc of the joint portion was 6200 A / mm 2 as a value calculated by the film thickness of the superconductor at the joint portion. In addition, the joining state of the joining portion was free from abnormal irregularities, foaming, different phases, etc. due to the flow of the high-temperature superconductor, and was well oriented parallel to the joining surface, and good joining was obtained.
【0025】比較例1 超電導複合体を突き合わせ、銀板の上部に形成した高温
超電導体間に高温超電導体前駆体(B)を接着した後の
加熱温度を864℃とした以外は実施例1と同様の工程
を経て高温超電導接合体を得た。得られた高温超電導接
合体の接合部とその周辺を顕微鏡及びX線回折法で観察
すると共に4端子法でJcを測定した。その結果、高温
超電導体の液体窒素温度77.3KでのJcは、接合前
は8600A/mm2及び接合後は8400A/mm2であり、ま
た接合部分のJcは、接合部分の超電導体膜厚さで算出
した値で800A/mm2と低かった。また接合部分は光沢
がなく、小さな凹凸を示し、超電導体の2212相結晶
は生成していたがごく微細であった。Comparative Example 1 The same as Example 1 except that the heating temperature after the superconducting composites were butted and the high temperature superconductor precursor (B) was bonded between the high temperature superconductors formed on the silver plate was 864 ° C. A high temperature superconducting joint was obtained through the same steps. The joint portion of the obtained high temperature superconducting joint and its periphery were observed by a microscope and an X-ray diffraction method, and Jc was measured by a four-terminal method. As a result, the Jc at the liquid nitrogen temperature 77.3K of high temperature superconductors, before joining the 8600A / mm 2 and after bonding are 8400A / mm 2, also Jc of the joint portion is, superconductor film thickness of the joint portion The calculated value was 800 A / mm 2 . Further, the joint portion was not glossy and showed small irregularities, and although the superconductor 2212 phase crystal was formed, it was very fine.
【0026】比較例2 超電導複合体を突き合わせ、銀板の上部に形成した高温
超電導体間に高温超電導体前駆体(B)を接着した後の
加熱温度を875℃とした以外は実施例1と同様の工程
を経て高温超電導接合体を得た。得られた高温超電導接
合体の接合部とその周辺を顕微鏡及びX線回折法で観察
すると共に4端子法でJcを測定した。その結果、高温
超電導体の液体窒素温度77.3KでのJcは、接合前
は8600A/mm2及び接合後は4300A/mm2であり、ま
た接合部分のJcは、接合部分の超電導体膜厚さで算出
した値で1200A/mm2と低かった上に、接合部分は高
温超電導体が溶けて流出し、高温超電導体の合計膜厚さ
100μmの設定値に対して約20μmに減少した。ま
た、異相(柱状結晶)が接合の境界に異常生成してい
た。Comparative Example 2 The same as Example 1 except that the superconducting composites were butted and the heating temperature after the high temperature superconductor precursor (B) was adhered between the high temperature superconductors formed on the silver plate was 875 ° C. A high temperature superconducting joint was obtained through the same steps. The joint portion of the obtained high temperature superconducting joint and its periphery were observed by a microscope and an X-ray diffraction method, and Jc was measured by a four-terminal method. As a result, the Jc at the liquid nitrogen temperature 77.3K of high temperature superconductors, before joining the 8600A / mm 2 and after bonding are 4300A / mm 2, also Jc of the joint portion is, superconductor film thickness of the joint portion The calculated value was as low as 1200 A / mm 2, and the high temperature superconductor melted and flowed out at the joint portion, and the total thickness of the high temperature superconductor was reduced to about 20 μm with respect to the set value of 100 μm. In addition, an abnormal phase (columnar crystal) was abnormally generated at the boundary of the joint.
【0027】実施例2 実施例1で得た超電導複合体から高温超電導体の部分だ
けを剥しとり、乳鉢で軽く粗砕して40μmの板状結晶
体を得た。次いで実施例1で得た高温超電導体前駆体
(A)70重量%に前記板状結晶体を30重量%添加し
たもの100重量部に、実施例1のグリーンシート
(A)を得る工程と同様の工程を経て厚さ170μmの
グリーンシート(C)(高温超電導体前駆体(C))を得
た。Example 2 Only the high temperature superconductor portion was peeled off from the superconducting composite body obtained in Example 1 and lightly crushed in a mortar to obtain a 40 μm plate crystal. Then, in the same manner as in the step of obtaining the green sheet (A) of Example 1, 100 parts by weight of 70% by weight of the high temperature superconductor precursor (A) obtained in Example 1 and 30% by weight of the plate-like crystal were added. Through the above process, a 170 μm thick green sheet (C) (high temperature superconductor precursor (C)) was obtained.
【0028】次に実施例1で得た超電導複合体を図2の
(a)及び(b)に示すように突き合わせ、かつ突き合
わせた双方の銀板1、1′の先端部を加締めて固定した
後、上記とは別の厚さ0.1mmの銀板6上に上記で得た
グリーンシート(C)、即ち高温超電導体前駆体(C)
7を60℃で10MPaの条件で熱圧着して複合材料5を
得た。次いで該複合材料5の高温超電導体前駆体(C)
の部分を下側にして、超電導複合体の高温超電導体2、
2′間の上部に載置し、しかる後大気中で870℃で3
0分間保持(加熱処理)し、その後850℃まで15時
間かけて降温し、更に20℃まで5時間かけて冷却して
高温超電導接合体を得た。なお冷却工程で680℃から
は雰囲気を窒素雰囲気に変更した。Next, the superconducting composite obtained in Example 1 is abutted as shown in FIGS. 2 (a) and 2 (b), and both ends of the abutted silver plates 1 and 1'are swaged and fixed. After that, the green sheet (C) obtained above, that is, the high temperature superconductor precursor (C), is placed on a silver plate 6 having a thickness of 0.1 mm, which is different from the above.
7 was thermocompression bonded at 60 ° C. under the condition of 10 MPa to obtain a composite material 5. Next, the high temperature superconductor precursor (C) of the composite material 5
With the part of the lower side facing down, the high-temperature superconductor 2 of the superconducting composite,
Place it on the upper part between 2'and then 3 at 870 ° C in the atmosphere.
After holding for 0 minutes (heat treatment), the temperature was lowered to 850 ° C. over 15 hours and further cooled to 20 ° C. over 5 hours to obtain a high temperature superconducting joint. In the cooling step, the atmosphere was changed to a nitrogen atmosphere from 680 ° C.
【0029】上記で得た高温超電導接合体の接合部とそ
の周辺を顕微鏡及びX線回折法で観察すると共に4端子
法でJcを測定した。その結果、高温超電導体の液体窒
素温度77.3KでのJcは、接合前は8600A/mm2
及び接合後は7900A/mm2であり、また接合部分のJ
cは、接合部分の超電導体膜厚さで算出した値で980
0A/mm2であった。また接合部の接合状態は、高温超電
導体の流動による異常な凹凸、発泡、異相等がなく、接
合面と並行に良く配向されており、良好な接合が得られ
ていた。The joint portion of the high-temperature superconducting joint body obtained above and its periphery were observed by a microscope and an X-ray diffraction method, and Jc was measured by a four-terminal method. As a result, the Jc of the high temperature superconductor at a liquid nitrogen temperature of 77.3K was 8600 A / mm 2 before joining.
And 7900 A / mm 2 after joining, and J
c is a value calculated from the thickness of the superconductor film at the joint portion, which is 980.
It was 0 A / mm 2 . In addition, the joining state of the joining portion was free from abnormal irregularities, foaming, different phases, etc. due to the flow of the high-temperature superconductor, and was well oriented parallel to the joining surface, and good joining was obtained.
【0030】実施例3 純度99.9重量%以上の酸化ビスマス(高純度化学研
究所製、3N)300g、炭酸ストロンチウム(高純度
化学研究所製、3N)147.6g、炭酸カルシウム
(高純度化学研究所製、3N)50.1g及び酸化第二
銅(高純度化学研究所製、3N)79.5gを秤量し、
合成樹脂製ボールミルに直径10mmの合成樹脂製ボール
1kg及び蒸留水500gと共に入れ72時間湿式混合し
た。混合物は100℃で24時間乾燥し、乾燥粉をジル
コニア容器に移し替えて、1050℃で2時間加熱後、
内容物を銀板上に流し出して急冷し、さらにらいかい機
で平均粒径8μmに乾式粉砕して溶融粉(B)を得た。Example 3 300 g of bismuth oxide (manufactured by Kojundo Chemical Laboratory, 3N) having a purity of 99.9% by weight or more, strontium carbonate (manufactured by Kojundo Chemical Laboratory, 3N) 147.6 g, calcium carbonate (manufactured by Kojundo Chemical) Weigh 50.1 g of 3N) made by R & D and 79.5 g of cupric oxide (3N made by Kojundo Chemical Laboratory),
1 kg of synthetic resin balls having a diameter of 10 mm and 500 g of distilled water were put into a synthetic resin ball mill and wet mixed for 72 hours. The mixture is dried at 100 ° C. for 24 hours, the dried powder is transferred to a zirconia container and heated at 1050 ° C. for 2 hours,
The contents were poured onto a silver plate, rapidly cooled, and further dry pulverized to an average particle size of 8 μm by a ladle machine to obtain a molten powder (B).
【0031】一方上記とは別に純度99.9重量%以上
の酸化ビスマス(高純度化学研究所製、3N)166
g、炭酸ストロンチウム(高純度化学研究所製、3N)
147.6g、炭酸カルシウム(高純度化学研究所製、
3N)50.0g及び酸化第二銅(高純度化学研究所
製、3N)79.6gを秤量し、合成樹脂製ボールミル
に直径10mmの合成樹脂製ボール1kg及び蒸留水500
gと共に入れ72時間湿式混合した。混合物は100℃
で24時間乾燥し、乾燥粉をジルコニア容器に移し替え
て、1050℃で2時間加熱後、内容物を銀板上に流し
出して急冷し、さらにらいかい機で平均粒径8μmに乾
式粉砕して溶融粉(C)を得た。On the other hand, separately from the above, bismuth oxide having a purity of 99.9% by weight or more (manufactured by Kojundo Chemical Laboratory, 3N) 166
g, strontium carbonate (manufactured by Kojundo Chemical Laboratory, 3N)
147.6 g, calcium carbonate (manufactured by Kojundo Chemical Laboratory,
3N) 50.0 g and cupric oxide (manufactured by Kojundo Chemical Laboratory Co., Ltd., 3N) 79.6 g are weighed, and 1 kg of synthetic resin balls having a diameter of 10 mm and distilled water 500 in a synthetic resin ball mill.
and wet mixed for 72 hours. The mixture is 100 ℃
For 24 hours, transfer the dried powder to a zirconia container, heat at 1050 ° C for 2 hours, then pour the contents onto a silver plate and quench, and further dry-mill to an average particle size of 8 μm with a raider machine. To obtain a molten powder (C).
【0032】さらにBi系2212相の理論組成になる
ように上記で得た溶融粉(B)を102.2g及び溶融
粉(C)を65.4gを秤量し、この溶融粉(B)及び
(C)100重量部にポリビニールブチラール樹脂(積
水化学製、商品名BL−2)5重量部、ジブチルフタレ
ート(和光純薬製、試薬一級)2重量部及びエチルアル
コール(和光純薬製、試薬一級)15重量部を添加して
混合した後、真空脱気して得られたスラリーを厚さが1
00μmのポリエステル製フィルム(東レ製)上に供給
し、ドクターブレード法でシート成形して厚さ170μ
mのグリーンシート(D)(高温超電導体前駆体(D))
を得た。Further, 102.2 g of the melted powder (B) and 65.4 g of the melted powder (C) obtained above were weighed so that the theoretical composition of the Bi type 2212 phase was obtained, and the melted powders (B) and ( C) 5 parts by weight of polyvinyl butyral resin (manufactured by Sekisui Chemical Co., Ltd., trade name BL-2), 2 parts by weight of dibutyl phthalate (manufactured by Wako Pure Chemical Industries, reagent first grade) and 100 parts by weight of ethyl alcohol (made by Wako Pure Chemical Industries, reagent first grade) ) 15 parts by weight were added and mixed, and then vacuum degassing was performed to obtain a slurry having a thickness of 1
It is supplied on a polyester film (made by Toray) of 00 μm and formed into a sheet by the doctor blade method to a thickness of 170 μm.
m green sheet (D) (high temperature superconductor precursor (D))
I got
【0033】この後厚さ0.1mmの銀板上に上記で得た
高温超電導体前駆体(D)を60℃で10MPaの条件で
熱圧着し、断面流速5cm/分で空気を流しながら焼成
し、高温超電導体前駆体(D)の一部が溶融し、かつ高
温超電導体結晶が得られる温度条件を調べた。その結
果、最高温度は864〜870℃の範囲で、保持時間は
2時間以内、降温速度は850℃以上は5℃/時間以下
が良好であることを確認した。Thereafter, the high-temperature superconductor precursor (D) obtained above was thermocompression-bonded on a silver plate having a thickness of 0.1 mm at 60 ° C. under the condition of 10 MPa, and fired while flowing air at a sectional flow rate of 5 cm / min. Then, a temperature condition under which a part of the high temperature superconductor precursor (D) was melted and a high temperature superconductor crystal was obtained was examined. As a result, it was confirmed that the maximum temperature was in the range of 864 to 870 ° C., the holding time was within 2 hours, and the cooling rate was 850 ° C. or higher and 5 ° C./hour or lower.
【0034】次に実施例1で得た超電導複合体を実施例
2と同様の方法で突き合わせ、かつ突き合わせた双方の
銀板の先端部を加締めて固定した後、上記とは別の厚さ
0.1mmの銀板上に上記で得たグリーンシート(D)、
即ち高温超電導体前駆体(D)を60℃で10MPaの条
件で熱圧着して複合材料を得た。次いで該複合材料の高
温超電導体複合体(D)の部分を下側にして、超電導複
合体の高温超電導体間の上部に載置し、以下加熱処理を
867℃で行った以外は実施例2と同様の工程を経て高
温超電導接合体を得た。Next, the superconducting composite obtained in Example 1 was abutted in the same manner as in Example 2, and the tips of both abutted silver plates were caulked and fixed, and then the thickness different from the above was applied. Green sheet (D) obtained above on a 0.1 mm silver plate,
That is, the high temperature superconductor precursor (D) was thermocompression bonded at 60 ° C. under the condition of 10 MPa to obtain a composite material. Then, the part of the high temperature superconductor composite (D) of the composite material was placed on the upper side between the high temperature superconductors of the superconducting composite, with the part of the high temperature superconductor composite (D) facing downward, and the following heat treatment was performed at 867 ° C. A high temperature superconducting junction was obtained through the same steps as described above.
【0035】上記で得た高温超電導接合体の接合部とそ
の周辺を顕微鏡及びX線回折法で観察すると共に4端子
法でJcを測定した。その結果、高温超電導体の液体窒
素温度77.3KでのJcは、接合前は8600A/mm2
及び接合後は8800A/mm2であり、また接合部分のJ
cは、接合部分の超電導体膜厚さで算出した値で630
0A/mm2であった。また接合部の接合状態は、高温超電
導体の流動による異常な凹凸、発泡、異相等がなく、良
好な接合が得られていた。The joint and the periphery thereof of the high temperature superconducting joint obtained above were observed by a microscope and an X-ray diffraction method, and Jc was measured by a four-terminal method. As a result, the Jc of the high temperature superconductor at a liquid nitrogen temperature of 77.3K was 8600 A / mm 2 before joining.
And 8800 A / mm 2 after joining, and J
c is a value calculated from the thickness of the superconductor film at the joint portion, which is 630.
It was 0 A / mm 2 . In addition, the joined state of the joined portion was free of abnormal irregularities, foaming, different phases, etc. due to the flow of the high-temperature superconductor, and good joining was obtained.
【0036】[0036]
【発明の効果】本発明の製造法によって得られる高温超
電導接合体は、接合する高温超電導体の超電導特性を低
下させることもなく、また接合部分の超電導体結晶も高
く配向させることができる為、良好な超電導接合が得ら
れる。さらに本発明によれば、高温超電導体の一部に欠
陥が生じ、高温超電導体で補修する必要が生じた場合に
も適用できる。EFFECTS OF THE INVENTION The high-temperature superconducting joint obtained by the manufacturing method of the present invention does not deteriorate the superconducting properties of the high-temperature superconductor to be joined, and the superconducting crystal at the joint can be highly oriented. A good superconducting junction can be obtained. Further, according to the present invention, it is possible to apply even when a defect occurs in a part of the high temperature superconductor and it is necessary to repair the high temperature superconductor.
【図1】(a)は本発明の一実施例になる高温超電導接
合体の製造作業状態を示す平面図及び(b)はその断面
図である。FIG. 1A is a plan view showing a manufacturing operation state of a high temperature superconducting assembly according to an embodiment of the present invention, and FIG. 1B is a sectional view thereof.
【図2】(a)は本発明の他の一実施例になる高温超電
導接合体の製造作業状態を示す平面図及び(b)はその
断面図である。FIG. 2A is a plan view showing a manufacturing operation state of a high temperature superconducting assembly according to another embodiment of the present invention, and FIG. 2B is a sectional view thereof.
1、1′ 銀板 2、2′ 高温超電導体 3 高温超電導体前駆体(B) 4 加締め部 5 複合材料 6 銀板 7 高温超電導体前駆体(C) 1, 1'Silver plate 2, 2'High temperature superconductor 3 High temperature superconductor precursor (B) 4 Crimped part 5 Composite material 6 Silver plate 7 High temperature superconductor precursor (C)
───────────────────────────────────────────────────── フロントページの続き (72)発明者 下田 修一郎 茨城県日立市東町四丁目13番1号 日立化 成工業株式会社茨城研究所内 (72)発明者 芦沢 寅之助 茨城県日立市東町四丁目13番1号 日立化 成工業株式会社茨城研究所内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Shuichiro Shimoda 4-13-1, Higashimachi, Hitachi, Ibaraki Prefecture Ibaraki Research Laboratory, Hitachi Chemical Co., Ltd. (72) Inventor Toranosuke Ashizawa 4-13, Higashimachi, Ibaraki No. 1 Hitachi Chemical Co., Ltd. Ibaraki Research Center
Claims (8)
接合する方法において、接合する高温超電導体間に高温
超電導体前駆体を介在させ、基材上に形成された高温超
電導体結晶が分解及び/又は溶融せず、かつ高温超電導
体前駆体の一部が溶融し、その後高温超電導体前駆体全
体が結晶化する温度で加熱して高温超電導体同士を接合
することを特徴とする高温超電導接合体の製造法。1. A method for joining high-temperature superconductors formed on a base material, wherein a high-temperature superconductor precursor is interposed between the high-temperature superconductors to be joined to form a high-temperature superconductor crystal formed on the base material. A high temperature characterized in that it does not decompose and / or melt, and that a part of the high-temperature superconductor precursor is melted, and then the whole high-temperature superconductor precursor is heated to a temperature at which the high-temperature superconductors are joined together. Superconducting junction manufacturing method.
超電導体前駆体が液状の高温超電導体前駆体を塗布した
もの又はシート状の高温超電導体前駆体を接合したもの
である請求項1記載の高温超電導接合体の製造法。2. The high-temperature superconductor precursor applied between the high-temperature superconductors to be joined is a liquid high-temperature superconductor precursor applied or a sheet-shaped high-temperature superconductor precursor joined. Method for manufacturing high temperature superconducting joints.
接合する方法において、貴金属板上に高温超電導体前駆
体の膜を形成して複合材料を得、次いで該複合材料の高
温超電導体前駆体の膜の部分を下側にして接合する高温
超電導体間の上部に載置した後、基材上に形成された高
温超電導体結晶が分解及び/又は溶融せず、かつ載置し
た高温超電導体前駆体の一部が溶融し、その後高温超電
導体前駆体全体が結晶化する温度で加熱して高温超電導
体同士を接合することを特徴とする高温超電導接合体の
製造法。3. A method for joining high-temperature superconductors formed on a base material to each other, wherein a film of a high-temperature superconductor precursor is formed on a noble metal plate to obtain a composite material, and then the high-temperature superconductor of the composite material. The high temperature superconductor crystal formed on the base material is not decomposed and / or melted after being placed on the upper part between the high temperature superconductors to be joined with the film portion of the precursor facing downward A method for producing a high temperature superconducting joined body, characterized in that a part of the superconductor precursor is melted and then heated at a temperature at which the whole high temperature superconductor precursor is crystallized to join the high temperature superconductors to each other.
導体と同じ結晶構造を有する高温超電導体結晶粉を50
重量%以下含有してなる請求項1、2又は3記載の高温
超電導接合体の製造法。4. A high-temperature superconductor crystal powder having the same crystal structure as that of the high-temperature superconductor to which the high-temperature superconductor precursor is to be bonded.
The method for producing a high temperature superconducting joint according to claim 1, 2 or 3, wherein the content is less than or equal to wt%.
Bi系高温超電導体2212相である請求項1、2、3
又は4記載の高温超電導接合体の製造法。5. The high-temperature superconductor and the high-temperature superconductor precursor are a Bi-based high-temperature superconductor 2212 phase.
Alternatively, the method for producing the high temperature superconducting assembly according to item 4.
合、仮焼して得たBi系の高温超電導体2212相組成
物である請求項1、2、3、4又は5記載の高温超電導
接合体の製造法。6. The high temperature superconductor according to claim 1, 2, 3, 4 or 5, wherein the composition of the high temperature superconductor precursor is a Bi-based high temperature superconductor 2212 phase composition obtained by mixing and calcining raw materials. Superconducting junction manufacturing method.
合、仮焼及び/又は溶融後粉砕した2種類以上の粉体を
さらに混合したBi系の高温超電導体2212相組成物
である請求項1、2、3、4又は5記載の高温超電導接
合体の製造法。7. The composition of the high-temperature superconductor precursor is a Bi-based high-temperature superconductor 2212 phase composition in which two or more kinds of powders obtained by mixing raw materials, calcining and / or melting and then pulverizing are further mixed. Item 6. A method for producing a high temperature superconducting joint according to item 1, 2, 3, 4 or 5.
板である請求項3、4、5、6又は7記載の高温超電導
接合体の製造法。8. The method for producing a high temperature superconducting assembly according to claim 3, 4, 5, 6 or 7, wherein the noble metal plate is silver or an alloy plate containing silver as a main component.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP32485894A JP3709999B2 (en) | 1994-11-24 | 1994-12-27 | Manufacturing method of high-temperature superconducting joints |
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6-289639 | 1994-11-24 | ||
| JP28963994 | 1994-11-24 | ||
| JP32485894A JP3709999B2 (en) | 1994-11-24 | 1994-12-27 | Manufacturing method of high-temperature superconducting joints |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH08203652A true JPH08203652A (en) | 1996-08-09 |
| JP3709999B2 JP3709999B2 (en) | 2005-10-26 |
Family
ID=26557671
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP32485894A Expired - Fee Related JP3709999B2 (en) | 1994-11-24 | 1994-12-27 | Manufacturing method of high-temperature superconducting joints |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3709999B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP2728592A4 (en) * | 2012-05-02 | 2015-09-23 | Furukawa Electric Co Ltd | SUPERCONDUCTING WIRE CONNECTION STRUCTURE, SUPERCONDUCTING WIRE CONNECTION METHOD, AND SUPERCONDUCTING WIRE FOR CONNECTION |
-
1994
- 1994-12-27 JP JP32485894A patent/JP3709999B2/en not_active Expired - Fee Related
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP2728592A4 (en) * | 2012-05-02 | 2015-09-23 | Furukawa Electric Co Ltd | SUPERCONDUCTING WIRE CONNECTION STRUCTURE, SUPERCONDUCTING WIRE CONNECTION METHOD, AND SUPERCONDUCTING WIRE FOR CONNECTION |
| US9502159B2 (en) | 2012-05-02 | 2016-11-22 | Furukawa Electric Co., Ltd. | Superconducting wire connection structure, superconducting wire connection method, and connection superconducting wire |
Also Published As
| Publication number | Publication date |
|---|---|
| JP3709999B2 (en) | 2005-10-26 |
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